Time resolved absorption and resonance Raman spectroscopic studies of the oxidation of benzidine in aqueous solution

We report a time resolved resonance Raman study of transient radicals produced in the pulse radiolytic oxidation of benzidine in aqueous solution. The intense and structured transient absorption in the 400–470 nm region, observed at microsecond times in the acidic medium, is attributed to the benzidine radical cation. The Raman spectrum, observed by excitation in resonance with this absorption, exhibits eight prominent bands which are assigned to planar phenyl vibrations. The ring breathing mode (v₁) at 844 cm^-1 is most highly resonance enhanced, indicating an overall expansion of the ring CC bonds in the excited state. The interring CC bond, with partial double bond character, is characterized by an intense (v₁₃) Raman band at 1335 cm^-1. The frequency of the in-phase v_7a CN stretching vibration is 1540 cm^-1. These frequencies and the presence of weak bands attributable to non-planar phenyl vibrations indicate the radical to be slightly non-planar. The pK_a for the proton loss from the radical cation is 10.87, four units higher than for the aniline radical cation. At high pH the observed transient has a broad and structureless absorption at ∽ 380 nm. It is identified from its resonance Raman features as the 4(4′aminophenyl)anilino radical formed by proton loss from the radical cation. The interring CC bond is characterized by a Raman band at 1292 cm^-1, indicating it to be a single bond. The structure of this neutral radical is highly nonplanar, with little conjugation between the two ring systems so that electronic excitation is primarily confined to the anilino moiety. The acidic and basic forms of the radical react rapidly in second order processes to produce products which absorb strongly at, respectively, 360 and 410 nm.     

Fast Raman spectroscopy of cytochrome c using intracavity resonance Raman amplification

The resonance Raman spectrum of cytochrome c (5 × 10^?4 M) was obtained using the method of resonance Raman amplification (RRA) in a dye laser resonator in 30 ns. The second harmonic of a Q-switched Nd glass laser was used as an excitation source and the spectra were recorded using a photographic plate.     

Resonance raman spectra and structure of p-aminoazobenzene dyes in diprotonated form

Resonance Raman spectra of methyl orange and its three ring deuterated and three ¹⁵N-azo derivatives have been measured in solutions in concentrated sulfuric acid and sulfuric acid-d₂. From the isotope shifts of the observed Raman bands, methylorange is confirmed to take the dicationic azo form protonated at the dimethylamino and the α-azo nitrogen atoms. The resonance Raman spectrum of tropaeolin OO is entirely different from that of methyl orange in concentrated sulfuric acid and is well elucidated on the basis of the protonated hydrazone-form, -NH-N⁺H =.     

Resonance Raman spectrum of the transient (SCN)−2 free radical anion

The resonance Raman spectrum of the transient species (λ_max = 475 nm, τ_{$\text{1}\text{2}$} = 1.6 μs) formed by pulse radiolysis of aqueous solutions of thiocyanate, SCN^2?, is reported. The spectrum is discussed in terms of the previous assignment of this transient to the radical anion, (SCN)^?₂. The observed vibrational frequencies of the radical anion are consistent with substantial weakening of the SS and the CN bonds are compared with neutral thiocyanogen.     

Near-infrared excitation of Raman scattering by chromophoric proteins

Fourier-transformed Raman spectra of bacteriorhodopsin, the photosynthetic reaction center, and myoglobin in aqueous solution excited at 1064 nm are presented. These proteins are representative of three important classes of chromophoric proteins. The observed vibrational modes are assigned and discussed based on the known resonance Raman spectra of these proteins. In each case, chromophore vibrations dominate the Raman scattering, with little or no contribution from other protein vibrations. However, the limitations encountered in resonance Raman studies of chromophoric proteins due to sample fluorescence or sample photolability are circumvented. The relative intensities in the bacteriorhodopsin Raman spectrum excited at 1064 nm are nearly identical to the relative intensities previously observed by resonance excitation. The Raman spectrum of the reaction center of the photosynthetic bacterium Rhodobacter sphaeroides excited at 1064 nm contains contributions from both bacteriochlorophyll and bacteriopheophytin pigments, with possible preresonance enhancement of bacteriochlorophyll modes. The 1064-nm-excited Raman spectrum of myoglobin displays several marker bands that have been characterized previously in resonance Raman investigations with excitation in both the Soret and Q-band regions.     

Stimulated Raman investigation of CO2-laser-excited SF6

Stimulated Raman spectroscopy is used to probe the photoexcitation dynamics of CO₂-laser-excited SF₆ in a molecular free-expansion jet. Time-dependent depletion of rotational levels in the ground state is observed by monitoring the ν₁ Raman spectrum at various delay times after the CO₂-laser excitation pulse. Optical Stark shifts are also seen, at short delay times, arising from resonances of the IR laser pulse with ν₃ transitions from both ground and ν₁ = 1 states. Molecules excited to the ν₃ = 1 level are detected by scanning the ν₁ + ν₃ ? ν₃ hot band. A direct determination of the anharmonicity X₁₃ = ?2.910 ± 0.002 cm^?1 is thus obtained.     

The resonance Raman spectra of intermediate-spin ferrous porphyrin

The resonance Raman and absorption spectra of unligated ferrous octaethylporphyrin [Fe²⁺ (OEP)] and its adduct with 2-MeIm or THF were observed. The resonance Raman spectrum of Fe²⁺ (OEP) in CH₂Cl₂ displayed characteristic features of iron porphyrin with three d_π electrons, suggesting ³E_g as the intermediate-spin (S = 1) ground state. Fe²⁺(OEP) in THF exhibited the ferrous high spin feature like Fe²⁺ (OEP) (2-MeIm) in CH₂Cl₂.     

Spectroscopic detection of excited-state electron transfer in porphyrin viologen systems

Pulsed laser excitation (354.7 nm, 10 ns pulse) of a pyridyltritolylporphyrin chromophore covalently linked to a dibenzylviologen, Bz₂V²⁺, electron acceptor (porphyrin—viologen, PV²⁺) in CH₃CN leads to intramolecular electron transfer quenching of the porphyrin singlet excited state within the laser pulsewidth to reduce the linked Bz₂V²⁺ to Bz₂V^+·. Transient Bz₂V^+· can be detected directly by resonance Raman spectroscopy. The same transient features are obtained from pulsed laser excitation of a mixture of porphyrin (P) and dibenzylviologen in CH₃CN where Bz₂V²⁺ quenches the porphyrin fluorescence, establishing bimolecular excited state electron transfer quenching to yield Bz₂V^+·. Confirmation of our assignment of the transient Bz₂V^+· comes from comparison of the spectra with the resonance Raman spectrum of an authentic sample of Bz₂V^+·, and of electrochemically reduced PV²⁺ which has been spectroscopically confirmed to form PV^+·. Fluorescence lifetime determinations for PV²⁺ and P yield a rate constant for intramolecular electron transfer, k_et = 8 × 10⁷ s⁻¹, consistent with the ability to observe electron transfer within the laser pulsewidth     

Observation of photodissociation of S2Cl2 and resonance Raman and fluorescence spectra of S2Cl under 514.5 nm radiation

The laser Raman spectrum of S₂Cl₂ varies with the sample temperature and/or the laser power. The Raman signals of S₂Cl₂ decreases as the sample molecules within the laser beam are dissociated by absorbing 514.5 nm photons. Above 540 K and 2 W of laser power, new resonance Raman and fluorescence bands appear. These bands were all assigned to S₂Cl. The fluorescence bands could be classified into two transition systems. Only one of them had the ground electronic state X̃ as its lower state. For the other, the low lying first excited state à was suspected. The fundamental frequencies suggested for the three vibrational modes were 664, 196 and 450 cm⁻¹ for the X̃ state and 630, 249 and 554 cm⁻¹ for the à state respectively.     

The vibrational spectrum and normal coordinate analysis of chlorodifluoromethane,CHClF2

The vibrational spectrum of chlorodifluoromethane has been reexamined. The i.r. and Raman spectra of the three isotopic species, ¹²CHClF₂, ¹³CHClF₂ and ¹²CDClF₂, have been obtained with better accuracy and higher resolution than in previous work. An SCF ab initio geometry optimization and quadratic force field calculation have been performed, and this force field has been further optimized to best fit the observed frequencies. The absorption spectrum of the ν₄, 2ν₆ region has been recorded at high resolution (0.002 cm⁻¹) and an analysis of the Fermi resonance perturbation has been carried out.     

Interferences in and lifetime measurement of a resonance electronic Raman effect using tunable pulsed laser techniques

The excitation profile for the intensity of electronic Raman transitions of terbium aluminum garnet (TbAlG) in the spectral range of 483.0–680.0 nm is reported. The electronic Raman transitions take place between the crystal field levels of the split ⁷F₆ ground manifold of TbAlG with shifts of 73 cm^?1 and 83 cm^?1 and the electronic Raman process is induced with tunable pulsed and fixed wavelength cw lasers. The tunability of the former was employed to obtain detailed information of the behaviour of the Raman intensity if the wavelength of the exciting source is tuned throughout the region of 483.0–490.0 nm where ⁵Da₄ ← ⁷F₆ absorptions of TbAlG occur and the data reveal the occurrence of interference effects. We also report measurements of the shape of the pulse — due to resonance enhanced electronic Raman scattered light — in real time. These studies reveal that the lifetime of the resonating state (which is responsible for the enhancement of the Raman intensity) as determined from the tailing end of the said pulse is within experimental error equal to the lifetime τ = 33.5 ± 1 μs of this state measured in a direct way from the intensity decay of an appropriate fluorescence transition of TbAlG.     

Guest-host interaction and photochemical transformation of silver particles isolated in rare gas matrices

Silver dimers and small clusters isolated in rare gas matrices are studied by UV-VIS absorption, emission, and resonance Raman spectroscopy. One, two, and three dimer trapping sites can be identified in Xe, Kr, and Ar matrices, respectively. The sites are identified by computer simulation to be either ofD _4h symmetry, with the molecules aligned in the 〈100〉-direction of thefcc-host lattice, or ofD _2h symmetry, with the molecules occupying single or double vacancies and aligned in the 〈110〉-direction. Low energy external modes of the dimers are observed in the resonance Raman spectra. They probe the guest-host interaction of the molecules and are assigned to librational modes. Trimers and larger clusters are found to be very photosensitive. Three different trimers can be observed in Xe and Kr matrices, respectively. They can be transformed reversibly into each other by laser irradiation. This indicates that probably three corresponding isomers can get stabilized in the two matrices. Further evidence for this interpretation is obtained from emission spectroscopy. Despite the photosensitivity of the trimers it is possible to stabilize the concentration of a particular species by a dual beam technique. Thus we obtained a resonance Raman spectrum of one species in a Xe matrix and a preresonance spectrum of the corresponding species in a Kr matrix.     

Low-frequency (20–400 cm−1) vibrational spectra of N-methylacetamide in the liquid state

Low-frequency Raman spectra (20–400 cm⁻¹) of liquid N-methylacetamide were studied. The experimental data were directly transformed into the R(v) representation. This spectrum was compared with the far infrared spectrum. Temperatures from 30 to 165 °C were investigated. A low-frequency band around 100 cm⁻¹ is assigned to a mode involving atoms in intermolecular hydrogen bonds. This assignment is qualitatively supported by the observed spectrum of Nd-methylacetamide.     

Resonanzramanspektrum von matrixisoliertem Se3

Resonance Raman Spectrum of Matrixisolated Se₃ By the application of a double furnace it is possible to get a gas mixture of 90% Se₂ molecules and 10% Se atoms. By condensing this mixture in an inertgas matrix at 15 K followed by annealing to nearly 25 K we got Se₃ molecules by a matrix reaction In the resonance Raman spectrum of this molecule we observed 14 overtones of the symmetric stretching vibration. So we can calculate the following values of ω₁ an x₁₁ for ⁸⁰Se₃: 312.15 ± 0.2 cm^?1 and 0.53 ± 0.02 cm^?1. Using a mixture of 62% ⁷⁶Se and 38% ⁸²Se we got band structures in which the intensity of the bands and their frequency shift can only be explained by a bent Se₃ molecule (～115°). The value of the force constant f_r + f_rr is 310 ± 20 Nm^?1. — By a new construction it is possible to get the Raman and IR reflection spectrum of the same matrix.     

Raman spectroscopic study of magnetite (FeFe2O4): a new assignment for the vibrational spectrum

A detailed Raman study on natural magnetite has been carried out. Raman spectra show four out of the five predicted Raman bands located at 668, 538, 306, and 193 rcm⁻¹. The location of the fifth, unobserved phonon mode, is inferred from spectra of other ferrites at 450-490 rcm⁻¹. Polarized experiments on an oriented single crystal provide a new interpretation of the Raman spectrum with the following assignment for symmetries of the observed modes: A_1g for 668 rcm⁻¹, E_g for 306 rcm⁻¹, and T_2g for 538, 193, and 450-490 rcm⁻¹. The results are compared with those of the earlier Raman studies and possible explanations for the discrepancies are suggested. Some of the inconsistencies can be resolved by considering the effect of oxidation of magnetite during the Raman experiments.     

Resonance-enhanced Raman scattering by aggregated 2,2′-cyanine on colloidal silver

The Raman scattering spectrum of 2,2′-cyanine on colloidal silver metal particles is discussed. Preliminary assignments of some of the vibrational Raman bands to the motions of specific chromophoric units are presented and multiplet character of some bands is discussed. Enhanced Raman scattering of 2,2′-cyanine occurs when the laser radiation is tuned to the J-aggregate absorption feature at 575 nm. The enhancement in Raman intensity is the result of a diminution of fluorescence intensity, as well as a quantitative increase in Raman scattering intensity, and is distinct from other types of enhancement phenomena (e.g., resonance Raman of monomeric solution dye, and surface-enhanced Raman scattering (SERS)). The resonance Raman enhancement, due to excitation at the frequency corresponding to the J-aggregate absorption, is found to be 2 × 10⁺³.     

Vibrational spectroscopic study of syngenite formed during the treatment of liquid manure with sulphuric acid

Syngenite (K₂Ca(SO₄)₂·H₂O), formed during treatment of manure with sulphuric acid, was studied by infrared, near-infrared (NIR) and Raman spectroscopy. C_s site symmetry was determined for the two sulphate groups in syngenite (P2₁/m), so all bands are both infrared and Raman active. The split ν₁ (two Raman+two infrared bands) was observed at 981 and 1000 cm⁻¹. The split ν₂ (four Raman+four infrared bands) was observed in the Raman spectrum at 424, 441, 471 and 491 cm⁻¹. In the infrared spectrum, only one band was observed at 439 cm⁻¹. From the split ν₃ (six Raman+six infrared) bands three 298 K Raman bands were observed at 1117, 1138 and 1166 cm⁻¹. Cooling to 77 K resulted in four bands at 1119, 1136, 1144 and 1167 cm⁻¹. In the infrared spectrum, five bands were observed at 1110, 1125, 1136, 1148 and 1193 cm⁻¹. From the split ν₄ (six infrared+six Raman bands) four bands were observed in the infrared spectrum at 604, 617, 644 and 657 cm⁻¹. The 298 K Raman spectrum showed one band at 641 cm⁻¹, while at 77 K four bands were observed at 607, 621, 634 and 643 cm⁻¹. Crystal water is observed in the infrared spectrum by the OH-liberation mode at 754 cm⁻¹, OH-bending mode at 1631 cm⁻¹, OH-stretching modes at 3248 (symmetric) and 3377 cm⁻¹ (antisymmetric) and a combination band at 3510 cm⁻¹ of the H-bonded OH-mode plus the OH-stretching mode. The near-infrared spectrum gave information about the crystal water resulting in overtone and combination bands of OH-liberation, OH-bending and OH-stretching modes.     

Transient Raman detection of excited state electron,transfer to methyl viologen from photoexcited molecular reagents in fluid solution and anchored to SiO2

The lowest electronic excited state of the complexes [Ru(2,2′-bipyridine)₃]²⁺, fac-[ClRe (CO)₃(2,2′-bipyridine)], and fac-[(pyridine) Re (CO)₃(2,2′-bipyridine)]⁺ can be quenched by methyl viologen, MV²⁺, N,N′-dimethyl-4,4′-bipyridinium, in fluid solutions. The quenching obeys Stern—Volmer kinetics as deduced from plots of relative luminescence quantum yield vs [MV²⁺], and the data are consistent with a quenching process that is essentially diffusion controlled. Pulsed laser excitation (18 ns, 354.7 nm frequency tripled Nd: YAG) of the metal complexes in the presence of MV²⁺ shows that a detectable fraction of the quenching results in net electron transfer to form MV⁺. The MV⁺ is detectable by resonance Raman scattering from the trailing portion of the excitation pulse. Excited state electron transfer to MV²⁺ from a photo-excited complex anchored to SiO₂ has also been detected by transient Raman spectroscopy. High surface area SiO₂ was functionalized by reaction with 4-[2-(trimethoxysilyl)ethyl]pyridine to give [SiO₂]-SiEtpyr. Reaction of [SiO₂]-SiEtpyr with [(CH₃CN)Re(CO)₃(2,2′-bipyridine)]⁺ then yields [SiO₂]-[(SiEtpyr) Re (CO)₃ (2,2′-bipyridine)]⁺. Electron transfer quenching of the photo-excited immobilized Re complex occurs when suspended in CH₃CN solutions of MV²⁺ to yield MV⁺ as detected by resonance Raman scattering and by lifetime attenuation in the presence of MV²⁺.     

Conformational study of 1,2-dithiacyclononane

The temperature dependence of the Raman spectrum of 1,2-dithiacyclononane (1,2-DTCN) in the SS stretching region has been used to infer the existence of a conformational equilibrium with ΔH⁰ = 5.0 ± 0.8 kJ/mol. Molecular mechanics calculations predict a (2 2 5)-C₂ lowest energy conformation in equilibrium with a (2 3 4) structure. The fully decoupled ¹³C NMR spectrum at −80°C and the Raman spectra are consistent with this postulate. The temperature dependence of the ¹H NMR spectrum of 1,2-DTCN is characteristic of the ring inversion process. A crude lineshape analysis allows us to calculate ΔG⁰ = 49.0 ± 1.2 kJ/mol.     

Theoretical study on the structures,force field,and vibrational spectra of cyclooctatetraene and cyclooctatetraene-d8

The structures and force field of 1,3,5,7-cyclooctatetraene (COT) have been studied using ab initio theory at the SCF level with the 4-21G basis set. The quadratic force field of the D_2d structure obtained by systematic scaling of the ab initio force constants successfully reproduces the observed frequencies of COT and COT-d₈ with a mean deviation of less than 10 cm⁻¹ for non-CH stretching modes. On the basis of the calculated results, assignments of the fundamental vibrations are examined. The normal mode υ₅ is reassigned to a weak band at 758 cm⁻¹ in the Raman spectrum of COT and to a weak band at 591 cm⁻¹ in the Raman spectrum of COT-d₈. The calculations favor the assignment of υ₂₆ given by Lippincott et al. [J. Am. Chem. Soc. 73, 3370 (1951)] over the revised assignment of Perec [Spectrochim. Acta 47A, 799 (1991)]. The calculations also furnish reliable prediction for the inactive A₂ fundamentals of COT and COT-d₈. The fundamental frequencies and IR and Raman intensities of ¹³CC₇H₈, which constitutes about 9% of COT in natural abundance, are also calculated. Only ν₁₀ (calculated at 908 cm⁻¹) of the formal inactive A₂ modes has appreciable Raman intensity (0.23 Å⁴/amu). A spectral feature due to this fundametal is identified in the liquid Raman spectrum of Tabacik and Blaise [C. R. Acad. Sci. Ser. II 303, 539 (1986)] as a weak peak at 908 cm⁻¹.